Specify the branch before defining a signed jump. Choose , and let be the value on the side with argument tending to from above, while is the value on the other side, with argument tending to from below. The entire function has the same limiting value on both sides, so
Thus the jump of a fractional power across a branch cut is
Equivalently the ratio of the limiting values is wherever is nonzero. Reversing the definition of the jump reverses its sign. Choosing a different branch multiplies both limits by the corresponding common phase.
The factor has algebraic branch points at zero and infinity. Near zero the leading behaviour is ; with , the behaviour near infinity is . These are four-sheeted branch points.
The polynomial denominator vanishes at , with nonzero derivative , and the fractional factor is finite and nonzero near either point on any chosen local branch. Hence
A single-valued holomorphic branch is obtained by choosing a branch cut joining zero to infinity. Points along the chosen cut mark its discontinuity, rather than additional isolated poles.
For this real integral choose , so the upper bank of the positive real axis has . Use a counterclockwise keyhole contour with inner radius and outer radius , enclosing . The upper-bank contribution tends to . On the lower bank, , and the reversed orientation makes its contribution .
The large arc is because , while the small arc is . Both vanish, giving
The residues on this branch are
The residue theorem yields
Therefore
The branch cut in (a) was arbitrary; here placing it on the integration axis makes the bank contributions directly proportional to the desired positive-real integral.

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